2.3

two dimensional motion (projectile motion)

a projectile is an object that moves under the influence of gravity alone. this results in a curved path called a parabolic trajectory.

projectile motion is analysed by resolving the motion into two independent components at right angles to each other.

horizontal component of motion

  • the horizontal component of velocity is written as v_x
  • there is no horizontal acceleration if air resistance is neglected
  • this means v_x remains constant throughout the motion
  • horizontal displacement can be found using x = v_x t

vertical component of motion

  • the vertical component of velocity is written as v_y
  • the vertical motion is affected by gravity
  • the acceleration is the acceleration of free fall, g
  • g acts downwards and has a value of approximately 9.81 ms⁻²

the horizontal and vertical motions are independent, but they share the same time of flight.

resolving the initial velocity

  • if the projectile is launched with speed u at an angle θ
  • horizontal component: u_x = u cos θ
  • vertical component: u_y = u sin θ

motion equations used in projectile problems

the standard equations of motion are applied separately to the horizontal and vertical directions.

  • vertical velocity: v_y = u_y + at
  • vertical displacement: s = u_y t + ½at²
  • horizontal displacement: x = v_x t

maximum height

  • at maximum height, the vertical velocity is zero: v_y = 0
  • this condition is used to calculate the time to reach maximum height
  • the vertical displacement equation is then used to find the maximum height

time of flight

  • the time to reach maximum height is half the total time of flight
  • total time of flight: t_total = 2t_max

horizontal range

  • the horizontal range is the total horizontal distance travelled
  • it is calculated using x = v_x t_total
  • the constant horizontal velocity simplifies the calculation